2 research outputs found
Measurements of Quarkonium Production and Polarization at CMS
The polarizations of Y(nS) (n=1,2,3) and prompt J/\psi and \psi(2S), as well
as the differential cross section of the Y(nS), are measured in proton-proton
collisions at sqrt(s) = 7 TeV, using a dimuon data sample collected by the CMS
experiment at the LHC, corresponding to an integrated luminosity of 4.9 fb-1.
The differential cross section is measured as a function of transverse momentum
of Y(nS). The data show a transition from exponential to power-law behavior in
the neighborhood of 20 GeV, and the power-law exponents for all three states
are consistent. The polarization parameters \lambda\theta, \lambda\phi, and
\lambda\theta\phi, as well as the frame-invariant quantity \lambda, are
measured from the dimuon decay angular distributions in three different
polarization frames. No evidence of large polarizations is seen in these
kinematic regions, which extend much beyond those previously explored.Comment: to appear in the proceedings of The 6th International Workshop on
Charm Physics (CHARM 2013
Measurements of Quarkonium production and polarization at CMS
Studies of quarkonium production and polarization play an important role in understanding QCD. CMS has recently measured the (nS) (n=1,2,3) production cross sections and polarizations, as well as the prompt (nS) (n=1,2) polarizations, using a dimuon sample collected in proton-proton collisions in 2011 at 7 TeV. The differential cross sections of the (nS) states are presented as a function of dimuon transverse momentum, covering a wide range of (10--100 GeV). All three states show a similar behaviour and display a change of shape from an exponential to a power-law at 20 GeV. The polarizations of the (nS) and (nS) states are determined in bins of dimuon transverse momentum and rapidity, significantly extending the and rapidity ranges probed by previous experiments. The experimental measurements are in disagreement with current theoretical predictions